In this section, we derive the general formalism for the EOS of ANM in \(d\) D space via the generalized HVH theorem [1]}.
We first briefly review the derivations in 3D and give the necessary ingredients [2]}, [3]}, [4]}, [5]}.
The single-nucleon potential \(U_J(\rho ,\delta ,|\mathbf {k}|)\)  (where \(J=\mathrm {n,p}\) ) could be expanded around \(\delta =0\)  as,
\(U_J(\rho ,\delta ,|\mathbf {k}|)\approx U_0(\rho ,|\mathbf {k}|)+U_{\mathrm {sym}}(\rho ,|\mathbf {k}|)\tau _3^J\delta +U_{\mathrm {sym,2}}(\rho ,|\mathbf {k}|)\delta ^2+\cdots ,\) 
